2000A&A...353..287A


Query : 2000A&A...353..287A

2000A&A...353..287A - Astronomy and Astrophysics, volume 353, 287-310 (2000/1-1)

The R Coronae Borealis stars - atmospheres and abundances.

ASPLUND M., GUSTAFSSON B., LAMBERT D.L. and RAO N.K.

Abstract (from CDS):

An abundance analysis of the H-deficient and He- and C-rich R Coronae Borealis (RCrB) stars has been undertaken to examine the ancestry of the stars. The investigation is based on high-resolution spectra and line-blanketed H-deficient model atmospheres. The models successfully reproduce the flux distributions and all spectral features, both molecular bands and high-excitation transitions, with one important exception, the Ci lines. Since photoionization of Ci dominates the continuous opacity, the line strengths of Ci are essentially independent of the adopted carbon abundance and stellar parameters. All predicted Ci lines are, however, much too strong compared with observations, with a discrepancy in abundance corresponding to 0.6dex with little star-to-star scatter. Various solutions of this ``carbon problem'' have been investigated. A possible solution is that classical model atmospheres are far from adequate descriptions of supergiants such as the RCrB stars. We can also not exclude completely, however, the possibility that the gf-values for the Ci lines are in error. This is supported by the fact that the Cii, [Ci] and C2 lines are reproduced by the models with no apparent complications. In spite of the carbon problem, various tests suggest that abundance ratios are little affected by the uncertainties. Judging by chemical composition, the RCrB stars can be divided into a homogeneous majority group and a diverse minority, which is characterized by extreme abundance ratios, in particular as regards Si/Fe and S/Fe. All stars show evidence of H- and He-burning in different episodes as well as mild s-process enhancements. Four of the majority members are Li-rich, while overabundances of Na, Al, Si and S are attributes of all stars. An anti-correlation found between the H and Fe abundances of H-deficient stars remains unexplained. These enigmatic stars are believed to be born-again giants, formed either through a final He-shell flash in a post-AGB star or through a merger of two white dwarfs. Owing to a lack of theoretical predictions of the resulting chemical compositions, identification of the majority and minority groups with the two scenarios is unfortunately only preliminary. Furthermore, Sakurai's object and V854 Cen exhibit aspects of both majority and minority groups, which may suggest that the division into two groups is too simplistic.

Abstract Copyright:

Journal keyword(s): stars: abundances - stars: evolution - stars: AGB and post-AGB - stars: variables: general - stars: individual: R CrB - stars: individual: Sakurai's object

VizieR on-line data: <Available at CDS (J/A+A/353/287): stars.dat table2.dat>

Simbad objects: 29

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Number of rows : 29
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* XX Cam RC* 04 08 38.7489702792 +53 21 39.350441448 8.35 8.10 7.27     F8I 139 0
2 HD 30353 sg* 04 48 53.3476200024 +43 16 32.086716960 8.05 8.22 7.76     A5Iap 142 0
3 V* SU Tau RC* 05 49 03.7301227728 +19 04 21.867600252   10.72 9.10     C1,0_Hd_CH0 151 1
4 V* UX Ant RC* 10 57 09.0588420456 -37 23 55.133370312   12.67 12.37     C-Hd 43 0
5 V* UW Cen RC* 12 43 17.1901954368 -54 31 40.763998596   10.84 10.13     K 115 0
6 V* Y Mus RC* 13 05 48.1948797744 -65 30 46.624502484   11.3 10.50     Fp_Hd 73 0
7 V* DY Cen RC* 13 25 34.0847063328 -54 14 43.129581792     12.00     C-Hd/B5-6Ie 96 0
8 V* V854 Cen RC* 14 34 49.4024471640 -39 33 19.201288284   7.13 11.69     Ce 208 0
9 V* R CrB RC* 15 48 34.4154827352 +28 09 24.295852440 6.44 6.31 5.71 5.26 5.08 G0Iep 779 0
10 HD 144941 pA* 16 09 24.5513020968 -27 13 38.184011148 9.45 10.17 10.02     B8 88 1
11 V* RT Nor RC* 16 24 18.6679360920 -59 20 38.565480480   11.34 10.60     R 80 0
12 V* RZ Nor RC* 16 32 41.66 -53 15 33.2     10.63     C-Hd 66 0
13 V* V652 Her pA* 16 48 04.6934854032 +13 15 42.420402252   10.31 10.51     ~ 137 0
14 V* V4334 Sgr CV* 17 52 32.69352 -17 41 08.0160           F2Ia 372 0
15 V* V3795 Sgr RC* 18 13 23.5642449000 -25 46 40.857266928       10.940 10.10 ~ 45 0
16 V* VZ Sgr RC* 18 15 08.5724613648 -29 42 29.491053228   11.15 10.46     ~ 53 0
17 V* RS Tel RC* 18 18 51.2223564000 -46 32 53.427456132   10.80 9.96     R0 79 1
18 V* GU Sgr RC* 18 24 15.5810208792 -24 15 26.353387944   11.40 11.33     R0 66 0
19 V* V348 Sgr pA* 18 40 19.9290428808 -22 54 29.308207716   12.1       B0/1?I?e 180 0
20 V* MV Sgr RC* 18 44 31.9665722184 -20 57 12.863610864 12.82 13.56 12.00 13.37   B2pec-Hd 105 0
21 V* FH Sct RC* 18 45 14.8470961608 -09 25 36.106185432           C 31 0
22 V* V CrA RC* 18 47 32.3096196393 -38 09 32.307864378       10.765   R0 107 0
23 V* V4732 Sgr Pu* 18 59 39.5771671848 -14 26 17.543500548 11.19 11.5 10.9     OB+ 36 0
24 V* RY Sgr RC* 19 16 32.7668605944 -33 31 20.340212592 6.20 6.27 6.25     Cpec 363 0
25 * ups Sgr Be* 19 21 43.6225957281 -15 57 18.062726294 4.18 4.71 4.61 4.34 4.21 B2Vp_sh 302 0
26 V* V482 Cyg RC* 19 59 42.5731664472 +33 59 27.937220100   12.91 11.36   9.029 C-Hd 68 0
27 V* FQ Aqr Pu* 20 51 21.3360113136 +02 18 46.360439064 9.18 9.62 9.52     F 63 0
28 V* U Aqr RC* 22 03 19.6990459464 -16 37 35.281076700   12.16 11.17     C-Hd 99 0
29 V* UV Cas RC* 23 02 14.6592341400 +59 36 36.693038052   11.89 11.80     F0/5Ib 62 0

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